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Question: Two conducting spheres of radii \(R_{1}\) and \(R_{2}\) carrying uniform volume charge densities \(+...

Two conducting spheres of radii R1R_{1} and R2R_{2} carrying uniform volume charge densities +ρ+\rho and ρ-\rho, respectively, are placed such that they partially overlap, as shown in the figure. At all points in the overlapping region:(this question has multiple correct options)

A. the electrostatic field is zero
B. the electrostatic potential is constant
C. the electrostatic field is constant in magnitude
D. the electrostatic field has same direction

Explanation

Solution

Electric field is the electric force due to a unit charge positive charge which is at rest exerted on its surrounding. We can find the electric field due to the individual charges and then sum them to find the electric field at the shaded region.
Formula: E=FqE=\dfrac{F}{q}orE=kqr2E=\dfrac{kq}{r^{2}}

Complete answer:
We know that the electric force due to a pair of charges is given by Coulomb's law. An electric field can be produced by a time-varying electric field or an electrical charge. These can be either attracting or repelling in nature.
An electric field E is defined as the electric force F per unit positive charge q, which is infinitesimally small and at rest, and is given as E=FqE=\dfrac{F}{q}. ThenE=kqr2E=\dfrac{kq}{r^{2}}, where k=14πϵ0k=\dfrac{1}{4\pi\epsilon_{0}} which is a constant and rr is the distance between the unit charges. Since the electric field is a vector quantity, it acts along the direction of the distance rr, then we can denote it as E=kqrr3\vec E=\dfrac{kq\vec r}{r^{3}}.
Here, we have two spheres, let +ρ+\rho be the volume density of the sphere R1R_{1} and, let ρ-\rho be the volume density of the sphere R2R_{2}. Let the distance between the two radii be dd.Then the charge q1q_{1} on R1R_{1} is given as +ρ43πR13+\rho\dfrac{4}{3}\pi R_{1}^{3} and the charge q2q_{2} on R2R_{2} is given as ρ43πR23-\rho\dfrac{4}{3}\pi R_{2}^{3}. If PP is point in the shaded region, let us assume that it is at a distance r1r_{1} and r2r_{2} from the radii R1R_{1} and R2R_{2} respectively.
Then, consider the figure shown, below.

Cleary, the electric field at PP is the superposition of the electric field vectors due to R1R_{1} and R2R_{2}, it is given as EP=K(+ρ43πR13)r1R13+K(ρ43πR23)r2R23=Kρ43π(r1r2)E_{P}=\dfrac{K\left(+\rho\dfrac{4}{3}\pi R_{1}^{3}\right)\vec r_{1}}{R_{1}^{3}}+\dfrac{K\left(-\rho\dfrac{4}{3}\pi R_{2}^{3}\right)\vec r_{2}}{ R_{2}^{3}}=K\rho\dfrac{4}{3}\pi(\vec r_{1}-\vec r_{2})
From the triangle in the figure, we can say that, d=r1r2d=r_{1}-r_{2} due to the vector addition .
Then, EP=Kρ43πdE_{P}=K\rho\dfrac{4}{3}\pi \vec d
Thus, we can say that the direction of the electric field is unchanged, i.e from positive to negative.

Thus the answer is D. the electrostatic field has same direction

Note:
Electric field is in the direction of the force. Usually, the electric field of a point positive charge is radially outwards, whereas the electric field of a point negative charge is radially inwards to the charge. However, the electric field also depends on the symmetry of the charge carrying conductor.